Magnitude of force acting on wedge and block

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SUMMARY

The discussion focuses on the conditions under which a block on a wedge will slip, specifically analyzing the force equation ##F = 0## and the relationship between the angle of the wedge (##\theta##), static friction coefficient (##\mu_s##), and the normal force (##n##). It is established that if the applied force ##F## exceeds a critical value of ##\frac{\tan\theta - \mu_s}{1+\mu_s \tan\theta}(M+m)g##, the block will not slip. The participants confirm the validity of this reasoning while acknowledging the ambiguity in the maximum and minimum force magnitudes discussed.

PREREQUISITES
  • Understanding of static friction and its coefficient (##\mu_s##)
  • Knowledge of forces acting on inclined planes
  • Familiarity with Newton's laws of motion
  • Basic grasp of trigonometric functions, particularly tangent (##\tan\theta##)
NEXT STEPS
  • Study the implications of varying the angle of inclination on static friction
  • Explore the derivation of the critical force equation for block and wedge systems
  • Investigate the effects of dynamic friction in similar scenarios
  • Learn about multi-directional forces and their impact on equilibrium in physics
USEFUL FOR

Physics students, mechanical engineers, and anyone studying the dynamics of forces on inclined surfaces will benefit from this discussion.

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Homework Statement
A block of mass m sits on a wedge of mass M, which is free to move along a horizontal surface with negligible friction. The coefficient of static friction between the block and the wedge is ##\mu_s##. A horizontal force of a magnitude ##F## pulls on the wedge, as shown in the attached diagram. When ##\tan \theta > \mu_s##, which of the following are true:

A) The force F must be directed to the right with a minimum magnitude.

B) The force F must be directed to the right with a maximum magnitude.

C) The block will slip even if ##F=0##.
Relevant Equations
Newton's second laws are crucial here. From drawing a free-body diagram, one can deduce that the static friction force ##f_s## satisfies ##f_s = m(g\sin \theta +\frac{F}{M+m} \cos\theta) \leq \mu_s m(g\cos\theta - \frac{F}{m+M} \sin\theta)## and that the required maximum force is ##\frac{\mu_s -\tan\theta}{1+\mu_s \tan\theta}(M+m)g ## (I'm stating this because the key part of this question is to determine which of the three statements are correct; I've already figured out the free-body diagrams and Newton's equations).
Clearly if ##F = 0## and ##\tan\theta > \mu_s##, then using the above equations for ##f_s## and ##n##, we get ##f_s > \mu_s n## so the block will slip. However, it seems that as long as the force ##F## is directed to the right with a certain minimum magnitude, namely ##\frac{\tan\theta - \mu_s}{1+\mu_s \tan\theta}(M+m)g##, the block won't slip.

Is this reasoning right?
 

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You have only considered one direction of slip, but I agree with your result.
Are you allowed to choose more than one option? It does say "are true", not "is true".
If it is supposed to be only one, I suspect it was intended to state the inequality the other way around.
 
Last edited:
Those maximum and minimum magnitudes seem ambiguous as a question.
 

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